lsm3241: bioinformatics and biocomputing lecture 6: fundamentals of molecular modeling prof. chen yu...
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LSM3241: Bioinformatics and LSM3241: Bioinformatics and BiocomputingBiocomputing
Lecture 6: Fundamentals of Molecular ModelingLecture 6: Fundamentals of Molecular Modeling
Prof. Chen Yu ZongProf. Chen Yu Zong
Tel: 6516-6877Tel: 6516-6877Email: Email: csccyz@nus.edu.sgcsccyz@nus.edu.sg
http://http://bidd.nus.edu.sgbidd.nus.edu.sgRoom 07-24, level 7, SOC1, Room 07-24, level 7, SOC1,
National University of SingaporeNational University of Singapore
22
Structural organization of a moleculeStructural organization of a molecule
Three features:
• Configuration (atom organization).
• Conformation (atom spatial arrangement).
• Shape (Surface landscape, steric packing)
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Structural organization of a moleculeStructural organization of a moleculeI. Configuration:
• The organization of atoms and chemical bonds. • Change of configuration requires breaking of bonds.
Switch between H and NH2 requires bond breaking.
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Structural organization of a moleculeStructural organization of a molecule
An important aspect of configuration is chirality
• Chirality defines the property of mirror image.
The image on the right is an mirror image of the one at left.
• If mirror image is not the same as the original, the compound is called chiral.
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Structural organization of a moleculeStructural organization of a molecule
Example of chiral and non-chiral compound:
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Structural organization of a moleculeStructural organization of a molecule
II. Conformation:
• Determined by the spatial positions of its constituent atoms.
• Inter-convertible without breaking and making bonds
Rotatable bond
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Protein structure and conformation change:Protein structure and conformation change:
Movie Show:
Drug Binding Induced Conformation Change in Protein
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Structural organization of a moleculeStructural organization of a molecule
III. Shape
• Steric packing (what part of space is covered by the compound).
• Surface features (cavities, grooves where other molecules can bind to).
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Protein Surface Determines Its Interaction with Protein Surface Determines Its Interaction with Other Molecules:Other Molecules:
Protein-Protein InteractionProtein-Protein Interaction
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Protein Surface Determines Its Interaction with Protein Surface Determines Its Interaction with Other Molecules:Other Molecules:
Protein-DNA InteractionProtein-DNA Interaction
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Protein Surface Determines Its Interaction with Protein Surface Determines Its Interaction with Other Molecules:Other Molecules:
Protein-RNA InteractionProtein-RNA Interaction
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Protein Surface Determines Its Interaction with Protein Surface Determines Its Interaction with Other Molecules:Other Molecules:
Protein-Drug InteractionProtein-Drug Interaction Mechanism of Drug Action:
A drug interferes with the function of a disease protein by binding to it.
This interference stops the disease process
Drug Design:
Structure of disease protein is very useful
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Atomic motions in a molecule Atomic motions in a molecule
• Atoms are not rigidly positioned.
• External and internal forces can induce atomic motions.
• Some motions have chemical effect. Movie Show:
Protein transient opening for ligand or drug binding and dissociation:
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Atomic motions in a molecule Atomic motions in a molecule
The effect of motions are described by energy:
Energy measures the ability to do work.
Motion is associated
with energy.
Movie Show:
Protein transient opening for ligand or drug binding and dissociation:
1515
Types of EnergyTypes of Energy Kinetic energy -- motional energy
Kinetic energy is related to the speed and mass of a moving object. The higher the speed and the heavier the object is, the bigger work it can do.
Potential Energy -- "positional" energy. Water falls from higher ground to lower ground. In physics such a phenomenon is
modeled by potential energy description:
Objects move from higher potential energy place to lower potential energy place.
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Potential Energy Description of Molecular MotionsPotential Energy Description of Molecular Motions A molecule changes from higher potential energy form to lower potential energy
form.
Potential energy is determined by inter-molecular, intra-molecular, and environmental forces
The total energy of motions is: Energy = Stretching Energy + Angle Bending Energy +Torsion Energy + Non-Bonded Interaction Energy
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The stretching energy equation is based on Hooke's law. The "kb" parameter controls the stiffness of the bond spring, while "ro" defines its equilibrium length.
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The stretching energy equation is based on Hooke's law. The "kb" parameter controls the stiffness of the bond spring, while "ro" defines its equilibrium length.
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The bending energy equation is also based on Hooke's law
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The bending energy equation is also based on Hooke's law
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The torsion energy is modeled by a simple periodic function
Why?
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Torsion energy as a function of bond rotation angle.
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
The non-bonded energy accounts for repulsion, van der Waals attraction, and electrostatic interactions.
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
• van der Waals attraction occurs at short range, and rapidly dies off as the interacting atoms move apart.
• Repulsion occurs when the distance between interacting atoms becomes even slightly less than the sum of their contact distance.
• Electrostatic energy dies out slowly and it can affect atoms quite far apart.
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Types of Hydrogen Bond:
N-H … ON-H … NO-H … NO-H … O
Can be modeled by
• VdW+electrostatic (AMBER)• Modified Linard-Jones (CHARM)• Morse potential (Prohofsky/Chen)
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Complete Energy Function:
bondednon ijij
ji
ij
ij
ij
ijrra
bondH
bondS
rra
rotationbond
n
eqbendinganglebond
eqrstretchbondatoms
r
r
B
r
AVeV
VeVn
v
krrkm
pH
][])1([
])1([)]cos(1[
2
)(2
1)(
2
1
2
61202)(
0
02)(
0
222
'0
'0
2727
Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Concept of energyscale is Important for molecular Modeling
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Concept of energy scale is Important for molecular modeling
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Molecular Modeling: Molecular Modeling: Basic Interactions and Their ModelsBasic Interactions and Their Models
Sources of force parameters:
Bonds, VdW, Electrostatic (for amino acids, nucleotides only):• AMBER: J. Am. Chem. Soc. 117, 5179-5197• CHARMM: J. Comp. Chem. 4, 187-217
H-bonds (Morse potential):• Nucleic Acids Res. 20, 415-419.• Biophys. J. 66, 820-826
Electrostatic parameters of organic molecules need to be computed individually by using special software (such as Gaussian)
bondednon ijij
ji
ij
ij
ij
ijrra
bondH
bondS
rra
rotationbond
n
eqbendinganglebond
eqrstretchbondatoms
r
r
B
r
AVeV
VeVn
v
krrkm
pH
][])1([
])1([)]cos(1[
2
)(2
1)(
2
1
2
61202)(
0
02)(
0
222
'0
'0
3030
Molecular Modeling: Molecular Modeling:
bondednon ijij
ji
ij
ij
ij
ijrra
bondH
bondS
rra
rotationbond
n
eqbendinganglebond
eqrstretchbondatoms
r
r
B
r
AVeV
VeVn
v
krrkm
pH
][])1([
])1([)]cos(1[
2
)(2
1)(
2
1
2
61202)(
0
02)(
0
222
'0
'0
Modeling Method I: Conformation search:
Change each torsion angle: Phi -> Phi+dphiSubsequent change of atom positions: xi -> xi+dxi; yi -> yi+dyi; zi -> zi+dziEnergy is changed: E -> E +dE
Each set of torsion angles corresponds to a conformation.Find sets with lower energy
All possible states can be explored
3131
Molecular Modeling: Molecular Modeling:
bondednon ijij
ji
ij
ij
ij
ijrra
bondH
bondS
rra
rotationbond
n
eqbendinganglebond
eqrstretchbondatoms
r
r
B
r
AVeV
VeVn
v
krrkm
pH
][])1([
])1([)]cos(1[
2
)(2
1)(
2
1
2
61202)(
0
02)(
0
222
'0
'0
Modeling Method II: Energy minimization:
Force guided approach:
Initialize: Change atom position: xi -> xi+dxi
Compute potential energy change: V -> V +dV
Determine next movement:
Force: Fxi=-dV/dxi; Fyi=-dV/dyi; Fzi=-dV/dziAtom displacement: dxi=C*FxiNew position: xi=xi+dxi
Energy minimization can only go down hill. Why?
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Summary of Today’s lectureSummary of Today’s lecture
• Structural organization of a molecule.• Basic interactions and models• Modeling methods (conformation search, energy
minimization)
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